The Plan dielectrics, quickly current & resistance HW3 hints after the break (& in lab) time...
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![Page 1: The Plan dielectrics, quickly current & resistance HW3 hints after the break (& in lab) time permitting, some of dc circuits.](https://reader035.fdocuments.in/reader035/viewer/2022070412/56649e975503460f94b9abb8/html5/thumbnails/1.jpg)
The Plan
• dielectrics, quickly
• current & resistance
• HW3 hints after the break (& in lab)
• time permitting, some of dc circuits
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Exam 1• Right here, 3pm Thursday
- electric forces & fields
- electrical potential & energy
- current & resistance
- NO RELATIVITY
• study quick quizzes, example probs
• our HW and quizzes
• problems in notesrelax.
it will be ok.
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not so funny now.
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battery = pumpvoltage = pressure
current = flowresistor = constriction
capacitor = diaphragm / flexible reservoirdiode = check valve
inductor = paddle wheel
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with the time left ...
let’s get a jump on dc circuits
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real battery = ideal battery + R
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actual circuit has a parasitic r
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real current sources
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
series resistors: conservation of energy
-+
R2
I I
∆V
R1a cbReq
∆V
a c
-+
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
voltage divider
R2
R1Vin Vout
Vout = R2
R1+R2Vin
signal in signal
out
R1
R2
volume
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
parallel resistors: conservation of charge
current divider
I
-+
R1
∆V
R2
a bI1
I2
∆V1=∆V2=∆V
-+
Req
∆V
Req R1 R2
1 11 = +
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
more complex arrangements
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measuring voltage
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real voltmeters
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measuring current
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a simple ammeter
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Thévenin equivalents
any weird combinations of R’s and V’sis equivalent
to aSINGLE R and V (or a single I source
in parallel with R)
Vth = V (open circuit)
Rth = V (open circuit)
I (closed circuit)
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
so what?
E
R
real sources = ideal sources + R
real meter = ideal meter with
R
VI R
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
V source loading
V
r
source
like a battery
Rload
∆Vload = V - Ir
for r ≪ Rload, ∆Vload ≈ V
V source wants R high
one easy solution:large resistor in parallel with load
I
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Ip
I source loading
source
Rload
I source wants R lowsourcing currents at high Rload is hard
Ir
Iload
Iload = Ir
r+R
for Rload ≪ r, Iload ≈ I
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
measuring the meter
Rload
I
Vr
realmeter
Req
I
V
idealmeter
∆Vload = IReq = R1+R/rI Rload ≪ r, ∆Vload ≈ IR
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
summary
voltmeter wants R low!can use a buffer/follower
I source wants R lowtransformer pre-ampconsider sourcing V
V source wants R highlarge series + parallel resistorspresent large R
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Sourcing current
Rwires
Rwires
RthingI V
This is what a hand meter does.
Why is it no good?
Vmeter = I(Rthing + 2Rwires)
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Sourcing current, properly
No problem.You just need four wires.
What is still wrong?
Rwires
Rwires
Rthin
g
I V
Rthing ≪ Rinternal
or add buffer
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Sourcing voltage
Rwires
Rwires
RthingVs
Still have to measure voltage on devicethe wires still use up some of V
What about current?
V
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
Sourcing voltage II
R = ∆V / I
Note we need 4 wires againcurrent meter - not hardstill problems?
Rwires
Rwires
Rthing
Vs
V
ΙΙ
=
Rprecise
V
RparRs
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
source/meter resistances
voltmeter wants R lowbut V source wants R high
need buffer/amp on V meter resistor in parallel with source
if V source is problem, R is too lowconsider sourcing I
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
what if I want to measure a *really* high R?
Rwires
Rwires
Rthing
Vs V
Ι
=Rs ≪ Rthing
Rp
Ι
=
V
source voltageRp has same voltage as Rthing
Rs has same current
have done >1010 Ohm
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
what if I want to measure a *really* low R?
Rwires
Rwires
Rthin
g
I V
this works just fine ...so long as your V meter is goodv. good amp / part of a bridge
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
what if I want to measure a small change in R?
V
R1 R3
R2 Rx+dR
Vs
balance bridge to V=0detect small changes from null
make R1-R3 about the sametrimming resistor on R2 = dR
R2 =
≈ R3
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center
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THE UNIVERSITY OF ALABAMA CENTER FOR MATERIALS FOR INFORMATION TECHNOLOGYAn NSF Science and Engineering Center